Chiral symmetry restoration at finite temperature in the planar limit

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dc.creatorNarayanan, R.
dc.creatorNeuberger, H.
dc.date2006-05-17
dc.date.accessioned2026-07-07T10:42:20Z
dc.date.available2026-07-07T10:42:20Z
dc.descriptionWe investigate numerically chiral symmetry restoration at finite temperature in the planar limit in the deconfined phase, both when it is stable and when the system is supercooled. We find chiral symmetry restoration at $T_χ= T_d$, where $T_d$ is the temperature of the deconfinement transition in pure gauge theory and $T_χ< T_d$ in the supercooled deconfined phase. In the stable case the spectrum of the Dirac operator opens a gap in a discontinuous manner and in the supercooled phase the gap seems to vanish continuously.
dc.description13 pages, 2 figures, one table, uses JHEP3.cls
dc.identifierhttps://arxiv.org/abs/hep-th/0605173
dc.identifierhttp://arxiv.org/abs/hep-th/0605173
dc.identifierPhys.Lett.B638:546-551,2006
dc.identifierdoi:10.1016/j.physletb.2006.05.081
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/181909
dc.subjectHigh Energy Physics - Theory
dc.subjectHigh Energy Physics - Lattice
dc.subjectHigh Energy Physics - Phenomenology
dc.titleChiral symmetry restoration at finite temperature in the planar limit
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